US3887395A - Cobalt-rare earth magnets comprising sintered products bonded with cobalt-rare earth bonding agents - Google Patents

Cobalt-rare earth magnets comprising sintered products bonded with cobalt-rare earth bonding agents Download PDF

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US3887395A
US3887395A US431127A US43112774A US3887395A US 3887395 A US3887395 A US 3887395A US 431127 A US431127 A US 431127A US 43112774 A US43112774 A US 43112774A US 3887395 A US3887395 A US 3887395A
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rare earth
cobalt
alloy
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Donald L Martin
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General Electric Co
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F1/00Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
    • H01F1/01Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
    • H01F1/03Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
    • H01F1/032Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of hard-magnetic materials
    • H01F1/04Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of hard-magnetic materials metals or alloys
    • H01F1/047Alloys characterised by their composition
    • H01F1/053Alloys characterised by their composition containing rare earth metals
    • H01F1/055Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5
    • H01F1/0555Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5 pressed, sintered or bonded together
    • H01F1/0557Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5 pressed, sintered or bonded together sintered
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B22CASTING; POWDER METALLURGY
    • B22FWORKING METALLIC POWDER; MANUFACTURE OF ARTICLES FROM METALLIC POWDER; MAKING METALLIC POWDER; APPARATUS OR DEVICES SPECIALLY ADAPTED FOR METALLIC POWDER
    • B22F7/00Manufacture of composite layers, workpieces, or articles, comprising metallic powder, by sintering the powder, with or without compacting wherein at least one part is obtained by sintering or compression
    • B22F7/02Manufacture of composite layers, workpieces, or articles, comprising metallic powder, by sintering the powder, with or without compacting wherein at least one part is obtained by sintering or compression of composite layers
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y10TECHNICAL SUBJECTS COVERED BY FORMER USPC
    • Y10STECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y10S264/00Plastic and nonmetallic article shaping or treating: processes
    • Y10S264/58Processes of forming magnets

Definitions

  • the present invention relates to the art of cobalt-rare earth alloy permanent magnets and more particularly it relates to the art of joining these magnets to produce magnets of desired large size or geometry without deleterious effect on magnetic properties.
  • Permanent magnets i.e., hard magnetic materials, such as the cobalt-rare earth alloys, are of technological importance because they can maintain a high, constant magnetic flux in the absence of an exciting magnetic field or electrical current to bring about such a field.
  • Cobalt-rare earth intermetallic compounds or alloys exist in a variety of phases.
  • cobalt-rare earth alloys containing a substantial amount of COSR in each occurrence R designates a rare earth metal
  • the bulk Co-R alloy must be reduced to a powder which 'is then usually compressed in an'aligning magnetic field to form an aligned pressed-powder compact.
  • the powder particles are magnetically aligned along their easy axis of magnetization prior to or during compaction since the greater their magnetic alignment, the better are the resulting magnetic properties.
  • the aligned pressed powder or green compact is sintered to produce a sintered body of the desired density.
  • a magnetizing field is applied to the sintered body parallel to its easy axis of magnetization, generally at room temperature, to produce a permanent magnet.
  • a disadvantage of this technique is that the sintered body or magnet is limited by the size of the pressedpowder or green compact.
  • the green compact itself, is limited in size because of the high pressure required to press the powder into a compact with sufficient strength so that it can be handled without excessive breakage before sintering.
  • a minimum pressure of about 100,000 psi is needed.
  • large magnets with an area greater than 4-5 square inches are difficult to make because of the need for presses greater than 200 tons.
  • the present process provides a method of bonding cobalt-rare earth alloy compacts without having any significant deleterious effect on the magnetic properties of the resulting bonded sintered magnet composite. Also, the bond in the composite is substantially as stable at elevated temperatures as the bonded sintered magnets. Specifically, the present bonding agent is a magnetic cobalt-rare earth alloy.
  • phase diagram at 300C which is the lowest temperature shown in the FIGURE, is substantially the same at room temperatures.
  • the present process comprises providing at least two compacts to be bonded together and sintered at a sintering temperature ranging from 900 C to l,250C.
  • Each compact consists essentially of compacted particulate permanent magnet alloy selected from the group consisting of Co-R, (Co-Fe)R, (Co-Cu)R, and (Co-Fe-Cu)R, where R is a rare earth metal or metals.
  • a layer of particles of a bonding magnet alloy agent is deposited on the bonding surface of one of the compacts, said agent being selected from the group consisting of Co-R, (Co-Fe)R, (Co-Cu)R, and (Co-Fe-Cu)R, where R is a rare earth metal or metals.
  • At least 1 percent by volume of the bonding agent passes through a liquid phase at an elevated temperature below sintering temperature or at sintering temperature and contains the rare earth metal component in a minimum amount of at least 10 atom higher than that contained in the compacts being bonded.
  • the bonding surface of the second compact is contacted with the deposited bonding agent substantially coextensively therewith, and the resulting assembly is sintered at a sintering temperature ranging from 900C to l,250C in an atmosphere in which it is substantially inert to bond and sinter said assembly to produce a solid composite sintered product having a density of at least 87%.
  • the present process comprises bonding at least two sintered products to form a solid bonded permanent magnet composite.
  • the process comprises providing at least two sintered permanent magnet products to be bonded, each said product having pores which are substantially non-interconnecting and a density of at least 87% and consisting essentially of sintered compacted particulate permanent magnet alloy selected from the group consisting of Co-R, (Co-Fe)R, (Co-Cu)R, and (Co-Fe-Cu)R, where R is a rare earth metal or metals.
  • a layer of particles of the bonding magnetic alloy agent is deposited on the bonding surface of one of the products, said agent being selected from the group consisting of Co-R, (Co-Fe)R, (Co-Cu)R, and (Co -Fe-Cu)R, where R is a rare earth metal or metals.
  • At least 1 percent by volume of the bonding agent passes through a liquid phase at an elevated temperature ranging up to l,250C and contains the rare earth metal component in a minimum amount of at least 10 atom higher than that contained in the sintered products being bonded.
  • the bonding surface of the second product is contacted with the deposited bonding agent substantially coextensively therewith, and the resulting assembly is heated to the elevated temperature ranging up to l,250C at which the bonding agent passes through the liquid phase.
  • the rare earth metals useful in forming the present bonding cobalt-rare earth alloy agent and the alloy or alloys of the present compacts or sintered products are the 15 elements of the lanthanide series having atomic numbers 57 to 71 inclusive.
  • the element yttrium (atomic number 39) is commonly included in this group of metals and, in this specification, is considered a rare earth metal.
  • a plurality of rare earth metals can also be used to form the present cobalt-rare earth alloys which, for example may be ternary, quartenary or which may contain an even greater number of rare earth metals as desired.
  • cobalt-rare earth alloys useful in the present invention are cobalt-cerium, cobaltpraseodymium, cobalt-neodymium, cobaltpromethium, cobalt-Samarium, cobalt-europium, cohalt-gadolinium, cobalt-terbium, cobalt-dysprosium, cobalt-holmium, cobalt-erbium, cobalt-thulium, cobalt-ytterbium, cobalt-lutecium, cobalt-yttrium, cobaltlanthanum and cobalt-mischmetal.
  • Mischmetal is the most common alloy of the rare earth metals which contains the metals in the approximate ratio in which they occur in their most common naturally occurring ores.
  • specific ternary alloys include cobalt-samarium-mischemetal, cobalt-ceriumpraseodymium, cobalt-yttrium-praseodymium, and cobalt-praseodymium-mischmetal.
  • each compact consists essentially of compacted particulate permanent magnet alloy selected from the group consisting of Co-R, (Co-Fe)R, (Co- Cu)R and (Co-Fe-Cu)R, where R is a rare earth metal or metals.
  • the permanent magnet alloy can be formed by a number of conventional methods and converted to particulate form in a conventional manner. Its particle size may vary and it can be in as finely divided a form as desired. For most applications, average particle size will vary from about 1 micron or less to about 10 microns.
  • the powder particles are magnetically aligned along their easy or preferred axis of magnetization prior to or during compression since the greater the magnetic alignment, the better are the resulting magnetic properties.
  • the aligned powder is pressed to a compact of desired size and shape. Compression can be carried out by a number of conventional techniques such as hydrostatic pressing or methods employing steel dies.
  • the density of the aligned compacts generally ranges from about 70% to 80% of theoretical.
  • the present bonding agent is an alloy selected from the group consisting of Co-R, (Co-Fe)R, (Co-Cu)R, and (Co-Fe-Cu)R, where R is a rare earth metal or metals.
  • the bonding agent is a solid at room temperature but at an elevated temperature ranging up to 1,250C at least 1 percent by volume of it, and preferably substantially all of it, passes through a liquid phase.
  • the agent can vary in composition and the specific elevated temperature at which it passes through a liquid phase in the required or desired amount can be determined from the phase diagram for the particular alloy system or it can be determined empirically.
  • the accompanying FIGURE shows that for the Co-Sm system, at a sintering temperature of l,lC, the present bonding agent contains Samarium in a minimum amount of about 26 atom
  • the present bonding agent is one which is at least atom and preferably higher than 10 atom richer in rare earth metal content than that contained in the compacts being bonded. This richer rare earth metal content is usually necessary for at least 1 percent by volume of the agent to pass through a liquid phase. Such liquid phase increases wetting and the extent of contact of the bonding agent with the bonding surfaces resulting in a strong bond being formed.
  • the bonding agent need not be composed of the same components as those of the alloys in the compacts being bonded.
  • a Co-Sm alloy bonding agent can be used to bond compacts of Co-Fe-Cu-Sm-Pr alloy. Since the magnetic properties of the bonding alloy agent diminish with diminishing amounts of the cobalt component, the maximum amount of rare earth component in the present bonding agent is atom When a significant amount of the bonding agent, i.e., above 10% by volume, does not pass through a liquid phase, it is preferably very fine in particle size so that when it is deposited on the bonding surfaces, it contacts a significant portion of the bonding surface area, preferably at least 50%.
  • the bonding surfaces of the compacts are not even or level but have a roughness corresponding to the projections of the compacted particles, and preferably, the fine-sized bonding agent particles will contact bonding surface between projections and thereby be in contact with a larger bonding surface area resulting in a stronger bond being formed.
  • the particle size of such a bonding agent preferably ranges from about 1 micron to 10 microns in size and particle sizes significantly higher than 10 microns do not provide sufficient contact with the bonding surfaces to produce a suitably bonded composite structure.
  • its particle size is not critical and can vary in the present invention.
  • a layer of the bonding alloy agent particles is deposited on a surface of one of the aligned compacts to be bonded. Since the aligned compact is somewhat magnetic, the deposited particles cling to its surface. The particular amount of the bonding agent deposited should be sufficient to result in a good bond in the composite product and is determinable empirically. Preferably, the bonding agent is deposited to form a continuous layer or deposit on the bonding surface. The surface of the second compact to be bonded is then placed in contact with the deposited layer substantially coextensively therewith.
  • the resulting assembly is heated to sintering temperature in an atmosphere in which it is substantially inert.
  • the aligned compacts are sufficiently magnetic so that the assembly holds together if maintained vertically, until the Curie temperature is reached and then just the weight of one compact on top of the other will hold it together during sintering.
  • the assembly can be supported or held together by conventional means such as a clamp.
  • the assembly is sintered in a substantially inert atmosphere to produce a solid sintered composite wherein the pores are substantially non-interconnecting, which generally is a sintered composite having a density of at least about 87% of theoretical.
  • Such non-interconnectivity stabilizes the permanent magnet properties of the composite product because its interior is protected against exposure to the ambient atmosphere.
  • the present permanent magnet type cobalt alloy systems require a sintering temperature ranging from 900 to 1,250C.
  • the particular sintering temperature depends largely on the particular cobalt alloy system being sintered. For example, for Co Sm type alloys, a
  • sintering temperature of l,lC is particularly satisfactory.
  • the sintered composite is cooled, preferably in an atmosphere in which it is substantially inert, preferably to room temperature
  • a magnetizing field is applied to the sintered composite along its easy axis of magnetization, preferably at room temperature, to produce a permanent magnet.
  • the density of the sintered composite may vary. The particular density depends largely on the particular permanent magnet properties desired. In the present invention, the density of the sintered composite ranges from about 87 to 100% of theoretical.
  • At least two sintered products are bondedtogether by the bonding agent.
  • the particles of bonding alloy are deposited on a surface of one of the sintered products and the bonding surface of the second sintered product is placed in contact with the deposited layer substantially coextensively therewith.
  • the resulting assembly is heated in an atmosphere in which it is substantially inert to an elevated temperature at which the bonding agent passes through the liquid phase up to 1,250C.
  • the solid composite of the present invention has a bond or joint which is visible to the naked eye.
  • This bond is magnetic so that it does not diminish the properties of the bonded magnets to any significant extent.
  • this bond is heat-stable, i.e., it is not significantly affected at the elevated temperatures at which the bonded magnets must be operable. Specifically, it is substantially as heat-stable as the bonded magnets, themselves.
  • a layer of particles of bonding alloy agent can be deposited on the bonding surface of each of a number of compacts or sintered products which can be stacked up, one upon the other, substantially coextensively with each other and sintered, or heated, or heatcompressed to form the desired bonded sintered composite structure.
  • the present method is useful for preparing large and- /or complex permanent magnet structures for such diverse applications as meters and instruments, magnetic separators, computers and microwave devices.
  • the invention is further illustrated by the following example.
  • EXAMPLE Particles of a 66.7 wt.% cobalt-33.3 wt.% samarium base alloy were admixed with particles of an additive 40 wt.% cobalt-6O wt.% samarium alloy to form a thorough mixture composed of 63 wt.% cobalt and 37 wt.% samarium.
  • the particles had an average size of about 6 microns.
  • a portion of the mixture was magnetically aligned along the easy axis by an aligning magnetizing field of 6O kiloersteds. After magnetic alignment, it was pressed to form a compact which was in theshape of a bar about 1 inch long and about /3 inch in diameter and had a packing about percent.
  • This sample which was the control sample, was sintered in an atmosphere of argon at a temperature of l,l20C for 1 hour, furnace-cooled to 875C where it was heat-aged for 5 hours and then cooled to room temperature in the same atmosphere.
  • the bonding alloy agent was composed of 40 wt.% cobalt-60 wt.% samarium and had a particle size of about 10 microns. All of this bonding agent passes through a liquid phase in the present example. This bonding agent was about 20 atom richer in samarium than that contained in the compacts being bonded.
  • the bonding surface of the second compact was contacted with the deposited bonding alloy agent substantially coextensively therewith to form an assembly in the form of a bar about 1 inch long.
  • the assembly was sintered at a temperature of l,l20C for 1 hour, then furnacecooled to a temperature of 875C where it was heataged for 5 hours and then quenched to room temperature in a helium atmosphere.
  • the bonded portion of the resulting composite appeared as an uneven thin line. The bonded portion of the composite appeared to be strong and did not break when force was applied manu ally.
  • a magnetizing field of 60 kiloersteds was applied at room temperature along the easy axis of magnetization to the control sample as well as the bonded composite and their magnetic properties were determined as shown in the following table where B, is the saturation induction,
  • B is the residual or remanent induction, i.e., the flux when the applied magnetic field is reduced to zero.
  • Normal coercive force H is the field strength at which the induction B becomes zero.
  • H helps characterize the squareness of the 4rrM demagnetization curve. Specifically, H, is the demagnetizing field required to drop the magnetization 10 percent below the remanence 8,. That is, 4'rrM 0.9 B,, and H is the corresponding field strength. H, is a useful parameter for evaluating demagnetization resistance.
  • the intrinsic coercive force H is the field strength at which the magnetization (B-H) or 41rM is zero.
  • the maximum energy product (Bl-1), represents the maximum product of the magnetic field H and the induction B determined on the demagnetization curve.
  • the present bonded composite has magnetic properties which are substantially the same as those of the control sample. This illustrates that the present bonding agent has no significant effect on the magnetic properties of the bonded magnets.
  • control sample and the bonded composite were then placed in an air oven maintained at 260C for about 24 hours and then cooled to room temperature in air. Force applied manually to the bonded portion of the composite indicated that heating in air at this elevated temperature did not weaken the bond.
  • the process comprises providing at least two compacts of particulate permanent magnet alloy, depositing a layer of particles of a bonding magnetic cobalt alloy agent on the bonding surface of one compact, contacting the bonding surface of the second compact with the deposited bonding agent substantially coextensively therewith, and sintering the resulting assembly to produce a sintered composite.
  • the bonding agent is a solid at sintering temperature.
  • a cobalt-rare earth alloy permanent magnet having an area greater than 4 square inches and substantially uniform permanent magnet properties throughout, said magnet consisting essentially of at least two sintered products bonded together by a magnetic bonding agent, each said sintered product consisting essentially of compacted particulate cobalt-rare earth permanent magnet alloy having pores which are substantially non-interconnecting and a density of at least 87%, said magnet being produced by depositing a layer of particles ranging in size up to 10 microns of a magnetic solid bonding agent on the bonding surface of one of said sintered products, said agent consisting essentially of cobalt-rare earth alloy containing the rare earth component in an amount at least 10 atom greater than that of the alloy of the sintered products being bonded with the maximum amount of rare earth component being 80 atom with at least 1% by volume of said agent passing through a liquid phase at an elevated temperature ranging up to 1,250C, contacting the bonding surface of the second sintered product with R is samarium.
  • said deposited bonding agent substantially coextensively therewith, and heating the resulting assembly in an atmosphere in which it'is substantially inert to a temperature at which said bonding agent passes through said liquid phase and ranging from 900 to 1,250C to bond said sintered products producing a solid bonded sintered product.
  • a cobalt-rare earth alloy permanent magnet having an area greater than 4 square inches and substantially uniform permanent magnet properties throughout, said magnet consisting essentially of a sintered product consisting essentially of at least two compacts bonded together by a magnetic bonding agent, each said compact being produced by providing a permanent magnet type alloy of cobalt and rare earth metal in particulate form having an average particle size up to about 10 microns, subjecting said particulate alloy to a magnetic field to align the particles along their easy axis of magnetization, and compressing said particulate alloy into a compact having a density of at least said sintered product being produced by depositing a layer of particles ranging in size up to 10 microns of a magnetic solid bonding agent on the bonding surface f0 one of said compacts, said agent consisting essentially of cobalt-rare earth alloy containing the rare earth component in an amount at least 10 atom greater than that of the alloy of each said compact with the maximum amount of rare earth component being atom with at least 1%

Abstract

Permanent cobalt alloy magnets of large size are prepared. At least two compacts of particulate permanent magnet cobalt alloy are provided and a layer of particles of a bonding magnetic cobalt alloy agent is deposited on the bonding surface of one compact. The bonding surface of the second compact is contacted with the deposited bonding agent substantially coextensively therewith and the resulting assembly is sintered to produce a sintered bonded composite. At least 1% by volume of the bonding agent passes through a liquid phase at an elevated temperature.

Description

United States Patent 1191 1111 3,887,395
Martin June 3, 1975 [5 COBALT-RARE EARTH MAGNETS 3,239,323 3/1966 Folweiler 65/43 COMPRISING SINTERED PRODUCTS 3,370,342 2/1968 Argyle et al. 29/4727 BONDED WITH COBALT RARE EARTH 3,655,464 4/1972 Benz 148/101 BONDING AGENTS Donald L. Martin, Elnora, N.Y.
General Electric Company, Schenectady, NY.
Jan. 7, 1974 Inventor:
Assignee:
Filed:
Appl. No.: 431,127
US. Cl. l48/3l.57; 29/470; 148/103; 148/105; 264/56; 264/DIG. 58
Int. Cl. H01f 1/04 Field of Search 148/3l.57, 101, 103, 105; 29/4727, 473.1, 470, DIG. 1; 264/56, DIG. 58; 65/43 References Cited UNITED STATES PATENTS 2/1966 Heimke et a1. l48/3l.57
Primary Examiner-Walter R. Satterfield Attorney, Agent, or FirmJane M. Binkowski; Joseph T. Cohen; Jerome C. Squillaro [5 7] ABSTRACT tensively therewith and the resulting assembly is sintered to produce a sintered bonded composite. At least 1% by volume of the bonding agent passes through a liquid phase at an elevated temperature.
4 Claims, 1 Drawing Figure COBALT-RARE EARTH MAGNETS COMPRISING SINTERED PRODUCTS BONDED WITH COBALT-RARE EARTH BONDING AGENTS The present invention relates to the art of cobalt-rare earth alloy permanent magnets and more particularly it relates to the art of joining these magnets to produce magnets of desired large size or geometry without deleterious effect on magnetic properties.
Permanent magnets, i.e., hard magnetic materials, such as the cobalt-rare earth alloys, are of technological importance because they can maintain a high, constant magnetic flux in the absence of an exciting magnetic field or electrical current to bring about such a field.
Cobalt-rare earth intermetallic compounds or alloys exist in a variety of phases. Thus far, cobalt-rare earth alloys containing a substantial amount of COSR (in each occurrence R designates a rare earth metal) have exhibited the best magnetic properties. However, to produce a permanent magnet with satisfactory properties, the bulk Co-R alloy must be reduced to a powder which 'is then usually compressed in an'aligning magnetic field to form an aligned pressed-powder compact. Specifically, the powder particles are magnetically aligned along their easy axis of magnetization prior to or during compaction since the greater their magnetic alignment, the better are the resulting magnetic properties.
The aligned pressed powder or green compact is sintered to produce a sintered body of the desired density. A magnetizing field is applied to the sintered body parallel to its easy axis of magnetization, generally at room temperature, to produce a permanent magnet.
A disadvantage of this technique is that the sintered body or magnet is limited by the size of the pressedpowder or green compact. The green compact, itself, is limited in size because of the high pressure required to press the powder into a compact with sufficient strength so that it can be handled without excessive breakage before sintering. Experience indicates that a minimum pressure of about 100,000 psi is needed. Thus, large magnets with an area greater than 4-5 square inches are difficult to make because of the need for presses greater than 200 tons.
One way of making a large magnet piece is to join smaller amounts together. Unfortunately, a suitable joining medium has not been found. Low temperature joining with solder or epoxy cement has been used to join cracked sintered pieces. The solder or epoxy joining method while attractive for many applications, limits the use of such bonded magnets at elevated temperature, particularly at temperatures in the range of 100 to 200C, which deteriorate these bonding agents and weaken the bond significantly. Also, materials such as solder or epoxy cement are non-magnetic thereby introducing an air gap which dilutes the magnetic properties of the joined magnets somewhat.
The present process provides a method of bonding cobalt-rare earth alloy compacts without having any significant deleterious effect on the magnetic properties of the resulting bonded sintered magnet composite. Also, the bond in the composite is substantially as stable at elevated temperatures as the bonded sintered magnets. Specifically, the present bonding agent is a magnetic cobalt-rare earth alloy.
Those skilled in the art will gain a further and better understanding of the present invention from the detailed description set forth below, considered in conjunction with the FIGURE accompanying and forming a part of the specification, which is the cobaltsamarium phase diagram. lt is assumed herein, that the phase diagram at 300C, which is the lowest temperature shown in the FIGURE, is substantially the same at room temperatures.
Briefly stated, the present process comprises providing at least two compacts to be bonded together and sintered at a sintering temperature ranging from 900 C to l,250C. Each compact consists essentially of compacted particulate permanent magnet alloy selected from the group consisting of Co-R, (Co-Fe)R, (Co-Cu)R, and (Co-Fe-Cu)R, where R is a rare earth metal or metals. A layer of particles of a bonding magnet alloy agent is deposited on the bonding surface of one of the compacts, said agent being selected from the group consisting of Co-R, (Co-Fe)R, (Co-Cu)R, and (Co-Fe-Cu)R, where R is a rare earth metal or metals. At least 1 percent by volume of the bonding agent passes through a liquid phase at an elevated temperature below sintering temperature or at sintering temperature and contains the rare earth metal component in a minimum amount of at least 10 atom higher than that contained in the compacts being bonded. The bonding surface of the second compact is contacted with the deposited bonding agent substantially coextensively therewith, and the resulting assembly is sintered at a sintering temperature ranging from 900C to l,250C in an atmosphere in which it is substantially inert to bond and sinter said assembly to produce a solid composite sintered product having a density of at least 87%.
Alternatively, the present process comprises bonding at least two sintered products to form a solid bonded permanent magnet composite. Specifically, in this alternative embodiment the process comprises providing at least two sintered permanent magnet products to be bonded, each said product having pores which are substantially non-interconnecting and a density of at least 87% and consisting essentially of sintered compacted particulate permanent magnet alloy selected from the group consisting of Co-R, (Co-Fe)R, (Co-Cu)R, and (Co-Fe-Cu)R, where R is a rare earth metal or metals. A layer of particles of the bonding magnetic alloy agent is deposited on the bonding surface of one of the products, said agent being selected from the group consisting of Co-R, (Co-Fe)R, (Co-Cu)R, and (Co -Fe-Cu)R, where R is a rare earth metal or metals. At least 1 percent by volume of the bonding agent passes through a liquid phase at an elevated temperature ranging up to l,250C and contains the rare earth metal component in a minimum amount of at least 10 atom higher than that contained in the sintered products being bonded. The bonding surface of the second product is contacted with the deposited bonding agent substantially coextensively therewith, and the resulting assembly is heated to the elevated temperature ranging up to l,250C at which the bonding agent passes through the liquid phase.
The rare earth metals useful in forming the present bonding cobalt-rare earth alloy agent and the alloy or alloys of the present compacts or sintered products are the 15 elements of the lanthanide series having atomic numbers 57 to 71 inclusive. The element yttrium (atomic number 39) is commonly included in this group of metals and, in this specification, is considered a rare earth metal. A plurality of rare earth metals can also be used to form the present cobalt-rare earth alloys which, for example may be ternary, quartenary or which may contain an even greater number of rare earth metals as desired.
Representative of the cobalt-rare earth alloys useful in the present invention are cobalt-cerium, cobaltpraseodymium, cobalt-neodymium, cobaltpromethium, cobalt-Samarium, cobalt-europium, cohalt-gadolinium, cobalt-terbium, cobalt-dysprosium, cobalt-holmium, cobalt-erbium, cobalt-thulium, cobalt-ytterbium, cobalt-lutecium, cobalt-yttrium, cobaltlanthanum and cobalt-mischmetal. Mischmetal is the most common alloy of the rare earth metals which contains the metals in the approximate ratio in which they occur in their most common naturally occurring ores. Examples of specific ternary alloys include cobalt-samarium-mischemetal, cobalt-ceriumpraseodymium, cobalt-yttrium-praseodymium, and cobalt-praseodymium-mischmetal.
In the present process at least two compacts are provided which are to be bonded together and sintered at a sintering temperature ranging from 900C to 1,250C. Each compact consists essentially of compacted particulate permanent magnet alloy selected from the group consisting of Co-R, (Co-Fe)R, (Co- Cu)R and (Co-Fe-Cu)R, where R is a rare earth metal or metals. The permanent magnet alloy can be formed by a number of conventional methods and converted to particulate form in a conventional manner. Its particle size may vary and it can be in as finely divided a form as desired. For most applications, average particle size will vary from about 1 micron or less to about 10 microns. Larger sized particles can be used but the maximum intrinsic coercive force obtainable is lower because it decreases with increasing particle size. The powder particles are magnetically aligned along their easy or preferred axis of magnetization prior to or during compression since the greater the magnetic alignment, the better are the resulting magnetic properties. The aligned powder is pressed to a compact of desired size and shape. Compression can be carried out by a number of conventional techniques such as hydrostatic pressing or methods employing steel dies. The density of the aligned compacts generally ranges from about 70% to 80% of theoretical.
The present bonding agent is an alloy selected from the group consisting of Co-R, (Co-Fe)R, (Co-Cu)R, and (Co-Fe-Cu)R, where R is a rare earth metal or metals. The bonding agent is a solid at room temperature but at an elevated temperature ranging up to 1,250C at least 1 percent by volume of it, and preferably substantially all of it, passes through a liquid phase. The agent can vary in composition and the specific elevated temperature at which it passes through a liquid phase in the required or desired amount can be determined from the phase diagram for the particular alloy system or it can be determined empirically. For example, the accompanying FIGURE shows that for the Co-Sm system, at a sintering temperature of l,lC, the present bonding agent contains Samarium in a minimum amount of about 26 atom Specifically, the present bonding agent is one which is at least atom and preferably higher than 10 atom richer in rare earth metal content than that contained in the compacts being bonded. This richer rare earth metal content is usually necessary for at least 1 percent by volume of the agent to pass through a liquid phase. Such liquid phase increases wetting and the extent of contact of the bonding agent with the bonding surfaces resulting in a strong bond being formed. The bonding agent need not be composed of the same components as those of the alloys in the compacts being bonded. For example, a Co-Sm alloy bonding agent can be used to bond compacts of Co-Fe-Cu-Sm-Pr alloy. Since the magnetic properties of the bonding alloy agent diminish with diminishing amounts of the cobalt component, the maximum amount of rare earth component in the present bonding agent is atom When a significant amount of the bonding agent, i.e., above 10% by volume, does not pass through a liquid phase, it is preferably very fine in particle size so that when it is deposited on the bonding surfaces, it contacts a significant portion of the bonding surface area, preferably at least 50%. Specifically, the bonding surfaces of the compacts are not even or level but have a roughness corresponding to the projections of the compacted particles, and preferably, the fine-sized bonding agent particles will contact bonding surface between projections and thereby be in contact with a larger bonding surface area resulting in a stronger bond being formed. Specifically, the particle size of such a bonding agent preferably ranges from about 1 micron to 10 microns in size and particle sizes significantly higher than 10 microns do not provide sufficient contact with the bonding surfaces to produce a suitably bonded composite structure. However, when substantially all of the bonding agent passes through a liquid phase, its particle size is not critical and can vary in the present invention.
In carrying out the process of the present invention, a layer of the bonding alloy agent particles is deposited on a surface of one of the aligned compacts to be bonded. Since the aligned compact is somewhat magnetic, the deposited particles cling to its surface. The particular amount of the bonding agent deposited should be sufficient to result in a good bond in the composite product and is determinable empirically. Preferably, the bonding agent is deposited to form a continuous layer or deposit on the bonding surface. The surface of the second compact to be bonded is then placed in contact with the deposited layer substantially coextensively therewith.
The resulting assembly is heated to sintering temperature in an atmosphere in which it is substantially inert. Frequently, the aligned compacts are sufficiently magnetic so that the assembly holds together if maintained vertically, until the Curie temperature is reached and then just the weight of one compact on top of the other will hold it together during sintering. However, if desired, the assembly can be supported or held together by conventional means such as a clamp.
The assembly is sintered in a substantially inert atmosphere to produce a solid sintered composite wherein the pores are substantially non-interconnecting, which generally is a sintered composite having a density of at least about 87% of theoretical. Such non-interconnectivity stabilizes the permanent magnet properties of the composite product because its interior is protected against exposure to the ambient atmosphere.
The present permanent magnet type cobalt alloy systems require a sintering temperature ranging from 900 to 1,250C. The particular sintering temperature depends largely on the particular cobalt alloy system being sintered. For example, for Co Sm type alloys, a
sintering temperature of l,lC is particularly satisfactory.
The sintered composite is cooled, preferably in an atmosphere in which it is substantially inert, preferably to room temperature A magnetizing field is applied to the sintered composite along its easy axis of magnetization, preferably at room temperature, to produce a permanent magnet.
The density of the sintered composite may vary. The particular density depends largely on the particular permanent magnet properties desired. In the present invention, the density of the sintered composite ranges from about 87 to 100% of theoretical.
Specifically, magnet compositions and sintering techniques particularly useful in the present invention are disclosed in U.S. Pat. Nos. 3,655,464; 3,655,463; and 3,695,945, all filed in the name of Mark G. Benz, and assigned to the assignee hereof, and all of which by reference are made part of the disclosure of the present application. Each of the aforementioned patents discloses a process for preparing novel sintered cobaltrare earth intermetallic products which can be magnetized to form permanent magnets having stable improved magnetic properties.
In the alternative embodiment of the present invention, at least two sintered products are bondedtogether by the bonding agent. In this instance the particles of bonding alloy are deposited on a surface of one of the sintered products and the bonding surface of the second sintered product is placed in contact with the deposited layer substantially coextensively therewith. The resulting assembly is heated in an atmosphere in which it is substantially inert to an elevated temperature at which the bonding agent passes through the liquid phase up to 1,250C.
The solid composite of the present invention has a bond or joint which is visible to the naked eye. This bond is magnetic so that it does not diminish the properties of the bonded magnets to any significant extent. Also, this bond is heat-stable, i.e., it is not significantly affected at the elevated temperatures at which the bonded magnets must be operable. Specifically, it is substantially as heat-stable as the bonded magnets, themselves.
If desired, a layer of particles of bonding alloy agent can be deposited on the bonding surface of each of a number of compacts or sintered products which can be stacked up, one upon the other, substantially coextensively with each other and sintered, or heated, or heatcompressed to form the desired bonded sintered composite structure.
The present method is useful for preparing large and- /or complex permanent magnet structures for such diverse applications as meters and instruments, magnetic separators, computers and microwave devices.
The invention is further illustrated by the following example.
EXAMPLE Particles of a 66.7 wt.% cobalt-33.3 wt.% samarium base alloy were admixed with particles of an additive 40 wt.% cobalt-6O wt.% samarium alloy to form a thorough mixture composed of 63 wt.% cobalt and 37 wt.% samarium. The particles had an average size of about 6 microns.
A portion of the mixture was magnetically aligned along the easy axis by an aligning magnetizing field of 6O kiloersteds. After magnetic alignment, it was pressed to form a compact which was in theshape of a bar about 1 inch long and about /3 inch in diameter and had a packing about percent. This sample, which was the control sample, was sintered in an atmosphere of argon at a temperature of l,l20C for 1 hour, furnace-cooled to 875C where it was heat-aged for 5 hours and then cooled to room temperature in the same atmosphere.
Two additional portions of the mixture were aligned and compacted in a substantially the same manner as the control sample to form two compacts, each of which were in the shape ofa bar about /2 inch long and A; inch in diameter and also having a packing of about 80 percent. The bonding surface of one of these compacts, i.e., the surface across the width thereof, was plunged into particles of a bonding alloy agent, and when it was removed therefrom, it had a substantially continuous layer of bonding agent particles clinging thereto.
The bonding alloy agent was composed of 40 wt.% cobalt-60 wt.% samarium and had a particle size of about 10 microns. All of this bonding agent passes through a liquid phase in the present example. This bonding agent was about 20 atom richer in samarium than that contained in the compacts being bonded. The bonding surface of the second compact was contacted with the deposited bonding alloy agent substantially coextensively therewith to form an assembly in the form of a bar about 1 inch long. The assembly was sintered at a temperature of l,l20C for 1 hour, then furnacecooled to a temperature of 875C where it was heataged for 5 hours and then quenched to room temperature in a helium atmosphere. The bonded portion of the resulting composite appeared as an uneven thin line. The bonded portion of the composite appeared to be strong and did not break when force was applied manu ally.
A magnetizing field of 60 kiloersteds was applied at room temperature along the easy axis of magnetization to the control sample as well as the bonded composite and their magnetic properties were determined as shown in the following table where B, is the saturation induction,
B, is the residual or remanent induction, i.e., the flux when the applied magnetic field is reduced to zero.
Normal coercive force H is the field strength at which the induction B becomes zero.
The term H helps characterize the squareness of the 4rrM demagnetization curve. Specifically, H, is the demagnetizing field required to drop the magnetization 10 percent below the remanence 8,. That is, 4'rrM 0.9 B,, and H is the corresponding field strength. H, is a useful parameter for evaluating demagnetization resistance.
The intrinsic coercive force H is the field strength at which the magnetization (B-H) or 41rM is zero.
The maximum energy product (Bl-1),, represents the maximum product of the magnetic field H and the induction B determined on the demagnetization curve.
As shown by the table, the present bonded composite has magnetic properties which are substantially the same as those of the control sample. This illustrates that the present bonding agent has no significant effect on the magnetic properties of the bonded magnets.
TABLE B 8,, H H),- rl )nm: Sample gauss gauss oers. oers. oers. l"gauss oers.) DensityiZ Alignment Control Sample 9,740 8,970 8,900 23,300 29,500 19.8 94.2 .977
Single Sintered Piece Bonded Sintered 9,720 9,030 8.800 21,400 29,000 19.8 95.0 .978
Composite The control sample and the bonded composite were then placed in an air oven maintained at 260C for about 24 hours and then cooled to room temperature in air. Force applied manually to the bonded portion of the composite indicated that heating in air at this elevated temperature did not weaken the bond.
in copending US. Pat. application Ser. No. 431,126 entitled Solid Bonding Agent for Cobalt-Rare Earth Alloy Magnets and Composite filed on even date herewith in the name of Donald L. Martin and assigned to the assignee hereof, and which by reference is made part of the disclosure of the present application, there is disclosed a process for producing sintered permanent magnets of large size. Briefly, the process comprises providing at least two compacts of particulate permanent magnet alloy, depositing a layer of particles of a bonding magnetic cobalt alloy agent on the bonding surface of one compact, contacting the bonding surface of the second compact with the deposited bonding agent substantially coextensively therewith, and sintering the resulting assembly to produce a sintered composite. The bonding agent is a solid at sintering temperature.
What is claimed is:
l. A cobalt-rare earth alloy permanent magnet having an area greater than 4 square inches and substantially uniform permanent magnet properties throughout, said magnet consisting essentially of at least two sintered products bonded together by a magnetic bonding agent, each said sintered product consisting essentially of compacted particulate cobalt-rare earth permanent magnet alloy having pores which are substantially non-interconnecting and a density of at least 87%, said magnet being produced by depositing a layer of particles ranging in size up to 10 microns of a magnetic solid bonding agent on the bonding surface of one of said sintered products, said agent consisting essentially of cobalt-rare earth alloy containing the rare earth component in an amount at least 10 atom greater than that of the alloy of the sintered products being bonded with the maximum amount of rare earth component being 80 atom with at least 1% by volume of said agent passing through a liquid phase at an elevated temperature ranging up to 1,250C, contacting the bonding surface of the second sintered product with R is samarium.
said deposited bonding agent substantially coextensively therewith, and heating the resulting assembly in an atmosphere in which it'is substantially inert to a temperature at which said bonding agent passes through said liquid phase and ranging from 900 to 1,250C to bond said sintered products producing a solid bonded sintered product.
2. A permanent magnet according to claim 1 wherein 3. A cobalt-rare earth alloy permanent magnet having an area greater than 4 square inches and substantially uniform permanent magnet properties throughout, said magnet consisting essentially of a sintered product consisting essentially of at least two compacts bonded together by a magnetic bonding agent, each said compact being produced by providing a permanent magnet type alloy of cobalt and rare earth metal in particulate form having an average particle size up to about 10 microns, subjecting said particulate alloy to a magnetic field to align the particles along their easy axis of magnetization, and compressing said particulate alloy into a compact having a density of at least said sintered product being produced by depositing a layer of particles ranging in size up to 10 microns of a magnetic solid bonding agent on the bonding surface f0 one of said compacts, said agent consisting essentially of cobalt-rare earth alloy containing the rare earth component in an amount at least 10 atom greater than that of the alloy of each said compact with the maximum amount of rare earth component being atom with at least 1% by volume of said agent passingthrough a liquid phase at an elevated temperature below or at sintering temperature, contacting the bonding surface of the second compact with said deposited bonding agent substantially coextensively therewith, and sintering and bonding the resulting assembly in an atmosphere in which it is substantially inert at a temperature at which said agent passes through said liquid phase ranging from 900 to 1,250C producing a solid sintered composite product having a density of at least 87%.
4. A permanent magnet according to claim 3 wherein R is samarium.

Claims (4)

1. A cobalt-rare earth alloy permanent magnet having an area greater than 4 square inches and substantially uniform permanent magnet properties throughout, said magnet consisting essentially of at least two sintered products bonded together by a magnetic bonding agent, each said sintered product consisting essentially of compacted particulate cobalt-rare earth permanent magnet alloy having pores which are substantially non-interconnecting and a density of at least 87%, said magnet being produced by depositing a layer of particles ranging in size up to 10 microns of a magnetic solid bonding agent on the bonding surface of one of said sintered products, said agent consisting essentially of cobalt-rare earth alloy containing the rare earth component in an amount at least 10 atom % greater than that of the alloy of the sintered products being bonded with the maximum amount of rare earth component being 80 atom % with at least 1% by volume of said agent passing through a liquid phase at an elevated temperature ranging up to 1,250*C, contacting the bonding surface of the second sintered product with said deposited bonding agent substantially coextensively therewith, and heating the resulting assembly in an atmosphere in which it is substantially inert to a temperature at which said bonding agent passes through said liquid phase and ranging from 900* to 1,250*C to bond said sintered products producing a solid bonded sintered product.
1. A COBALT-RARE EARTH ALLOY PERMANENT MAGNET HAVING AN AREA GREATER THAN 4 SQUARE INCHES AND SUBSTANTIALLY UNIFORM PERMANENT MAGNET PROPERTIES THROUGHOUT, SAID MAGNET CONSISTING ESSENTIALLY OF AT LEAST TWO SINTERED PRODUCTS BONDED TOGETHER BY A MAGNETIC BONDING AGENT, EACH SAID SINTERED PRODUCT CONSISTING ESSENTIALLY OF COMPACTED PARTICULATE COBALT-RARE EARTH PERMANENT MAGNET ALLOY HAVING PORES WHICH ARE SUBSTANTIALLY NON-INTERCONNECTING AND A DENSITY OF AT LEAST 87%, SAID MAGNET BEING PRODUCED BY DEPOSITING A LAYER OF PARTICLES RANGING IN SIZE UP TO 10 MICRONS OF A MAGNETIC SOLID BONDING AGENT ON THE BONDING SURFACE OF ONE OF SAID SINTERED PRODUCTS, SAID AGENT CONSISTING ESSENTIALLY OF COBALT-RARE EARTH ALLOY CONTAINING THE RARE EARTH COMPONENT IN AN AMOUNT AT LEAST 10 ATOM % GREATER THAN THAT OF THE ALLOY OF THE SINTERED PRODUCTS BEING BONDED WITH THE MAXIMUM AMOUNT OF RARE EARTH COMPONENT BEING 80 ATOM % WITH AT LEAST 1% BY VOLUME OF SAID AGENT PASSING THROUGH A LIQUID PHASE AT AN ELEVATED TEMPERATURE RANGING UP TO 1,250*C, CONTACTING THE BONDING SURFACE OF THE SECOND SINTERED PRODUCT WITH SAID DEPOSITED BONDING AGENT SUBSTANTIALLY COEXTENSIVELY THEREWITH, AND HEATING THE RESULTING ASSEMBLY IN AN ATMOSPHERE IN WHICH IT IS SUBSTANTIALLY INERT TO A TEMPERATURE AT WHICH SAID BONDING AGENT PASSES THROUGH SAID LIQUID PHASE AND RANGING FROM 900* TO 1,250*C TO BOND SAID SINTERED PRODUCTS PRODUCING A SOLID BONDED SINTERED PRODUCT.
2. A permanent magnet according to claim 1 wherein R is samarium.
3. A cobalt-rare earth alloy permanent magnet having an area greater than 4 square inches and substantially uniform permanent magnet properties throughout, said magnet consisting essentially of a sintered product consisting essentially of at least two compacts bonded together by a magnetic bonding agent, each said compact being produced by providing a permanent magnet type alloy of cobalt and rare earth metal in particulate form having an average particle size up to about 10 microns, subjecting said particulate alloy to a magnetic field to align the particles along their easy axis of magnetization, and compressing said particulate alloy into a compact having a density of at least 70%, said sintered product being produced by depositing a layer of particles ranging in size up to 10 microns of a magnetic solid bonding agent on the bonding surface fo one of said compacts, said agent consisting essentially of cobalt-rare earth alloy containing the rare earth component in an amount at least 10 atom % greater than that of the alloy of each said compact with the maximum amount of rare earth component being 80 atom % with at least 1% by volume of said agent passing through a liquid phase at an elevated temperature below or at sintering temperature, contacting the bonding surface of the second compact with said deposited bonding agent substantially coextensively therewith, and sintering and bonding the resulting assembly in an atmosphere in which it is substantially inert at a temperature at which said agent passes through said liquid phase ranging from 900* to 1, 250*C producing a solid sintered composite product having a density of at least 87%.
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US4076561A (en) * 1976-10-15 1978-02-28 General Motors Corporation Method of making a laminated rare earth metal-cobalt permanent magnet body
US4174966A (en) * 1978-12-15 1979-11-20 The United States Of America As Represented By The Secretary Of The Interior High coercive force rare earth metal-cobalt magnets containing copper and magnesium
US4224067A (en) * 1979-04-27 1980-09-23 The United States Of America As Represented By The Secretary Of The Army Permanent magnet materials
US4710239A (en) * 1984-09-14 1987-12-01 General Motors Corporation Hot pressed permanent magnet having high and low coercivity regions
US4762574A (en) * 1985-06-14 1988-08-09 Union Oil Company Of California Rare earth-iron-boron premanent magnets
US4818305A (en) * 1980-12-18 1989-04-04 Magnetfabrik Bonn Gmbh Process for the production of elongated articles, especially magnets, from hard powdered materials
US4933009A (en) * 1985-06-14 1990-06-12 Union Oil Company Of California Composition for preparing rare earth-iron-boron-permanent magnets
US4952252A (en) * 1985-06-14 1990-08-28 Union Oil Company Of California Rare earth-iron-boron-permanent magnets
US20030110617A1 (en) * 1999-12-22 2003-06-19 Reppel Georg Werner Method for producing rod-shaped permanent magnets

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Cited By (11)

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Publication number Priority date Publication date Assignee Title
FR2326017A1 (en) * 1975-09-23 1977-04-22 Bbc Brown Boveri & Cie PERMANENT MAGNET AND ITS PRODUCTION PROCESS
US4076561A (en) * 1976-10-15 1978-02-28 General Motors Corporation Method of making a laminated rare earth metal-cobalt permanent magnet body
US4174966A (en) * 1978-12-15 1979-11-20 The United States Of America As Represented By The Secretary Of The Interior High coercive force rare earth metal-cobalt magnets containing copper and magnesium
US4224067A (en) * 1979-04-27 1980-09-23 The United States Of America As Represented By The Secretary Of The Army Permanent magnet materials
US4818305A (en) * 1980-12-18 1989-04-04 Magnetfabrik Bonn Gmbh Process for the production of elongated articles, especially magnets, from hard powdered materials
US4710239A (en) * 1984-09-14 1987-12-01 General Motors Corporation Hot pressed permanent magnet having high and low coercivity regions
US4762574A (en) * 1985-06-14 1988-08-09 Union Oil Company Of California Rare earth-iron-boron premanent magnets
US4933009A (en) * 1985-06-14 1990-06-12 Union Oil Company Of California Composition for preparing rare earth-iron-boron-permanent magnets
US4952252A (en) * 1985-06-14 1990-08-28 Union Oil Company Of California Rare earth-iron-boron-permanent magnets
US20030110617A1 (en) * 1999-12-22 2003-06-19 Reppel Georg Werner Method for producing rod-shaped permanent magnets
US6926777B2 (en) * 1999-12-22 2005-08-09 Vacuumschmelze Gmbh & Co. Kg Method for producing rod-shaped permanent magnets

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